Time needed for velocity to become v<vf: t = (1/gy) ln (Vf/v) + (Vf/v) - 1

AI Thread Summary
The discussion centers on calculating the time required for a particle falling through the air to reach a velocity less than its terminal velocity (vf). The initial acceleration of the particle is equal to gravitational acceleration (g) but decreases until it reaches zero, at which point the particle falls at terminal velocity. To determine the time for the velocity to become less than vf, explicit integrations of the varying acceleration are necessary, as opposed to using simple kinematic equations. The equations presented involve integrating the acceleration function and setting up the appropriate limits for velocity and time. The conversation emphasizes the need for integral forms due to the changing nature of acceleration during the fall.
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1. When a particle falls though the air, its initial acceleration a=g diminishes until it is zero, and thereafter it falls at a constant or terminal velocity vf. If the variation of the acceleration can be expressed as a=(g/v^2f)(v^2f-V62), determine the time needed for the velocity to become v<vf. Initially the particle falls from rest.

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s4orce said:
determine the time needed for the velocity to become v<vf. Initially the particle falls from rest.

Do you mean find the time for the velocity to become v=vf? v will be < vf all the way up until the particle reaches terminal velocity.

And to solve the problem, you will need to do the explicit integrations. The only reason that the simple kinematic equations of motion do not have integrals in them is becuase the acceleration is constant with time. When it is changing, you need to use the integral forms of those equations. Can you show us how you would set those up?
 
It is v< (less than) vf.

What I have thus far is

a=g(Vf^2-V2^2/Vf^2)

a=g(1-(V2^2/Vf^2)

Integral 0 to V (1/1-(V^2/Vf^2) dv=Integral 0 to T gdt

1/2 ln V+Vf/V-Vs=gt

t=1/gy ln V+Vt/V-Vt

dv/dt=g(1-V^2/Vf^2)

1/2a ln v+a/v-a

1/2 ln V/Vf+1 / V/ Vx-1 Integral 0 to V gt
 
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